TY - JOUR
T1 - The growth of matter perturbations in
AU - Gannouji, R.
AU - Moraes, B.
AU - Polarski, D.
PY - 2009
Y1 - 2009
N2 - We consider the linear growth of matter perturbations on low redshifts in some f(R) dark energy (DE) models. We discuss the definition of dark energy (DE) in these models and show the differences with scalar-tensor DE models. For the f(R) model recently proposed by Starobinsky we show that the growth parameter γ 0≡γ(z = 0) takes the value γ 0 0.4 for Ω m,0 = 0.32 and γ 0 0.43 for Ω m,0 = 0.23, allowing for a clear distinction from ΛCDM. Though a scale-dependence appears in the growth of perturbations on higher redshifts, we find no dispersion for γ(z) on low redshifts up to z ∼ 0.3, γ(z) is also quasi-linear in this interval. At redshift z = 0.5, the dispersion is still small with Δγ 0.01. As for some scalar-tensor models, we find here too a large value for γ′ 0≡(dγ/dz)(z = 0), γ′ 0 -0.25 for Ω m,0 = 0.32 and γ′ 0 -0.18 for Ω m,0 = 0.23. These values are largely outside the range found for DE models in General Relativity (GR). This clear signature provides a powerful constraint on these models. 2009 IOP Publishing Ltd and SISSA.
AB - We consider the linear growth of matter perturbations on low redshifts in some f(R) dark energy (DE) models. We discuss the definition of dark energy (DE) in these models and show the differences with scalar-tensor DE models. For the f(R) model recently proposed by Starobinsky we show that the growth parameter γ 0≡γ(z = 0) takes the value γ 0 0.4 for Ω m,0 = 0.32 and γ 0 0.43 for Ω m,0 = 0.23, allowing for a clear distinction from ΛCDM. Though a scale-dependence appears in the growth of perturbations on higher redshifts, we find no dispersion for γ(z) on low redshifts up to z ∼ 0.3, γ(z) is also quasi-linear in this interval. At redshift z = 0.5, the dispersion is still small with Δγ 0.01. As for some scalar-tensor models, we find here too a large value for γ′ 0≡(dγ/dz)(z = 0), γ′ 0 -0.25 for Ω m,0 = 0.32 and γ′ 0 -0.18 for Ω m,0 = 0.23. These values are largely outside the range found for DE models in General Relativity (GR). This clear signature provides a powerful constraint on these models. 2009 IOP Publishing Ltd and SISSA.
KW - Cosmological perturbation theory
KW - Dark energy theory
UR - http://www.scopus.com/inward/record.url?scp=65649124529&partnerID=8YFLogxK
U2 - 10.1088/1475-7516/2009/02/034
DO - 10.1088/1475-7516/2009/02/034
M3 - Article
AN - SCOPUS:65649124529
SN - 1475-7516
VL - 2009
JO - Journal of Cosmology and Astroparticle Physics
JF - Journal of Cosmology and Astroparticle Physics
IS - 2
M1 - 034
ER -